Electrostatic extraction method and apparatus for cyclotrons

ABSTRACT

A method and apparatus for electrostatically extracting high beam currents at improved energy from small diameter, high magnetic field cyclotrons by deflecting particles from their trajectory within an electrostatic field traversing an extraction channel wherein magnetic material immediately adjacent to the inside of at least a portion of the channel first reduces the fringe field and then reverses its normal gradient to assist in extraction and to focus the extracted beam radially with respect to the center of the cyclotron.

United States Patent [191 Hendry May 13, 1975 [54] ELECTROSTATIC EXTRACTION METHOD 3,582,700 6/1971 Hendry 328/234 3,624,527 11/1971 Hudson 3l3/62 AND APPARATUS FOR CYCLOTRONS [75] Inventor: George 0. Hendry, Napa, Calif.

[73] Assignee: The Cyclotron Corporation,

Berkeley, Calif.

[22] Filed: Dec. 8, 1972 [2]] Appl. No.: 313,451

[52] US. Cl 313/62; 328/234 [51] Int. Cl. H05] 13/08 [58] Field of Search 313/62; 328/234; 250/495 ME [56] References Cited UNITED STATES PATENTS 3,382,391 5/1968 Reich .L 313/62 3,398,308 8/1968 Steimel 313/62 Primary Examiner-James W. Lawrence Assistant Examiner-B. C. Anderson [5 7] ABSTRACT A method and apparatus for electrostatically extracting high beam currents at improved energy from small diameter, high magnetic field cyclotrons by deflecting particles from their trajectory within an electrostatic field traversing an extraction channel wherein magnetic material immediately adjacent to the inside of at least a portion of the channel first reduces the fringe field and then reverses its normal gradient to assist in extraction and to focus the extracted beam radially with respect to the center of the cyclotron.

3 Claims, 4 Drawing Figures PATENTED HAY 1 31975 3.883 .761

sum 10F 2 MAGNETIC FIELD B RADIUS FIG 4 1 ELECTROSTATIC EXTRACTION METHOD AND APPARATUS FOR CYCLOTHRONS.

This invention relates generally to beam extraction from cyclotrons and moreparticularly to a method and means for extracting a high-energy high quality beam from small diameter isochronous cyclotrons.

One object of this invention is toincrease the amount and quality of beam current available from a small diameter, high magnetic field isochronous cyclotron.

Another object of this invention is to provide a method and means for enabling electrostatic deflection of a beam of higher energy particles from an isochronous cyclotron of any fixed diameter.

Other objects and advantages of this invention will become apparent from a consideration of the following description in connection with the accompanying drawings wherein,

FIG. 1 is a partially schematic cross-sectional view of a typical isochronous cyclotron at its median plane;

FIG. 2 is a plan view of the electrostatic deflection assembly of this invention;

1 FIG. :3 is a cross-sectional view of a portion of the electrostatic deflection assembly taken along line 3 3 of FIG. 2; and I FIG. 4 is a curve plotting fringe magnetic field strength (B) of the cyclotron against radius in the region of the extraction radius.

This invention relates to electrostatic extraction methods and apparatus, for example, like those known for isochronous cyclotrons generally disclosed in U.S.

Pat. No. 3,582,700 entitled Cyclotron Beam Extraction System and in copending application Ser. No. 1 18,751 entitled Improved Cyclotron Beam Extraction filed on Feb. 25, 1971 by George 0. Hendry and Dale K. Wells, now U.S. Pat. No. 3,725,709. The external beam current of the isochronous cyclotrons therein described for a fixed cyclotron diameter can be produced at higher energy, increased in amount and improved in quality by the present invention wherein magnetic material is placed along at least a portion of the electrostatic deflection channel. The magnetic material concentrates the lines of magnetic force of the fringe field of the cyclotron, first to reduce that field at the electrostatic deflection channel and thereby assist in deflection and second to reverse the fringe field gradient so I that it tends to focus the extracted beam of particles radially with respect to the center of the cyclotron.

FIG. 1 illustrates the orientation of the electrostatic deflection assembly of this invention with respect to the other components of a typical small isochronous cyclotron at its median plane. A main d-c electromagnet defines a magnetic guide field for the particles orbiting within the evacuated region of the cyclotron. The main d-c magnet includes a lower yoke slab 2, a pair of interconnecting iron legs 3 and two cylindrical iron pole bases 4, the lower one of which is shown in FIG. 1. In the described embodiment the lower pole tip is warp plate 6b that, with sidewalls and with a similar upper warp plate, forms a vacuum tank Within which charged particles are accelerated in the machine.

Three shaped hill pieces 9 mount on each of the warp plates in corresponding locations to produce the azimuthally varying field necessary for isochronous operation. A pair of hollow 120 dees within the vacuum tank provides a radio frequency accelerating field and an ion source supplies ions for acceleration in the central region of the cyclotron between the two dees all as is more fully described in U.S. Pat. No. 3,582,700.

In the described embodiment the extraction system includes electrostatic deflection means 30 and a mag netic channel 31 which receives and radially focuses a beam of ions deflected by the electrostatic deflection I means. Also a preseptum unit 50 mounts adjacent to the electrostatic deflection means 30 at the extraction radius and precedes it with respect to the path of orbiting particles as is more fully described in copending application Ser. No. 118,751 now U.S. Pat. No. 3,725,709.

FIGS. 2-3 show the improved electrostatic deflection assembly of this invention in detail. It includes a thin curved tungsten septum 35 maintained at ground potential and a curved deflector electrode 36 which is held at a high negative potential (for positively charged, accelerated particles). The septum 35 and deflector electrode 36 define between them a shaped electrostatic deflection channel 37 with a high electric field gradient which is located so it increases in radius with respect to the center of the cyclotron. When traversed by the orbiting particles segregated by the preseptum 50, the electrostatic field forces the particles to move to a larger radius where they no longer are held in a circular path by the main magnet.

The septum and deflector electrode are carefully shaped and located so that the segregated beam remains centered in the channel as it moves to greater radius. Both mount upon a water cooled non-magnetic base plate 38 on one of the hill pieces 9 as shown in FIG. 1. The septum 35 clamps to the base plate 38 and an upper cooling plate 39. A pair of alumina insulators 46 cantilevered from brackets 47 support the hollow copper deflector electrode 36 from base plate 38. Electrode 36 is cooled by water coolant supplied to its interior through hollow electrical conductor 48a and returned through conductor 48b. The same conductors 48a, 48b provide high negative potential to the electrode from its power supply.

After leaving the electrostatic channel 37 the beam of extracted particles follows a path of increasing radius and is focused radially by magnetic channel 31.

While output beam currents in the order of 50 microamperes of 22 MeV protons can be obtained in a 30 inch cyclotron with the described electrostatic deflection means alone, an improvement in external beam energy for the same cyclotron diameter in the order of 50 microamperes at 30 MeV protons can be obtained by placement of magnetic material inside at least a portion of the electrostatic deflection channel 37. As is more particularly shown in Figs. 2 and 3, this magnetic material can be in the form of an iron bar 60 clamped to septum 35 at its terminal end from which the extracted beam leaves channel 37. In the described embodiment, for example, iron bar 60 is secured to the septum 35 by a pair of clamps 61 to which it is held by cap screws 62.

The presence of the magnetic material concentrates the lines of force of the fringe magnetic field of the machine through it, first to reduce the fringe field just radially beyond it and to assist the electrostatic-deflection and second to reverse the gradient of the fringe field and focus the extracted particles radially with respect to the center of the cyclotron.

For example, in FIG. 4 the curve shown in solid lines depicts the normal fringe magnetic field (B) plotted against the machine radius in the region of the extraction radius. At the entrance to the electrostatic channel 37, the electric field across it normally reduces the net fringe field as shown in the vertical portion 71 of the curve 70. The net field then has a normally reducing gradient as at 72 of the same slope as the fringe field would have without the effect of the uniform elec-. trostatic field. At the terminal end of the channel the electrostatic field no longer has any effect and the net fringe field returns verticallly at 73 to its normal value along curve 74.

With the magnetic material of this invention in place, however, the normal fringe field in the region of the extraction radius is modified as shown in hidden lines in FIG. 4. The net field increases as at 80, then drops vertically along 71 to a value 81 less than that normally reached without the iron in place. Then, the normally decreasing gradient through the channel at 72 is reversed so that, as'one moves radially, the net field has an increasing gradient as at 82 to the end of the channel where the curve resumes the same shape 73 as in normal operation.

The specific iron placement of this invention is shown for illustrative purposes only. The iron bar may vary in size or shape or may extend further along the septum. In practice it has been found that the iron should extend as far as possible along the channel to produce the effects described, but should not be so long as to have the internally orbiting particles impinge upon it which are not segregated by the septum and preseptum and directed through the electrostatic channel. Those and various other modifications will be apparent to those skilled in the art within the scope of the invention defined in the following claims.

I claim:

1. Improved apparatus for electrostatically deflecting a beam of charged particles at an extraction radius in the fringe magnetic field of an isochronous cyclotron comprising means defining an electrostatic field across a deflection channel at the extraction radius, the location of said field'increasing in radius with respect to the center of the cyclotron; and magnetic material positioned inside and adjacent to at least a portion of said channel to reduce the cyclotron fringe field at the channel and to focus the beam of charged particles radially with respect to the center of the cyclotron, by concentrating the lines of magnetic force of said fringe field inwardly of but immediately adjacent to said channel to reduce said fringe field and then to reverse the nor- 1 mally decreasing field gradient in said channel.

2. The apparatus of claim 1 wherein the means defining an electrostatic field includes a thin curved septum and a curved deflector electrode which define between them a shaped deflection channel with a high electric field gradient across it and the magnetic material is positioned along inside of at least a portion of said septum.

3. An improved method for electrostatically deflecting a beam of charged particles at an extraction radius in the fringe magnetic field of an isochronous cyclotron comprising the steps of defining an electrostatic field within a channel at the extraction radius which increases in radius with respect to the center of the cyclotron; and

placing a magnetic member along at least a portion of said channel to concentrate the lines of magnetic force of said fringe field inwardly of but immediately adjacent to said channel to reduce said fringe field and then to reverse the normally decreasing field gradient in said channel. 

1. Improved apparatus for electrostatically deflecting a beam of charged particles at an extraction radius in the fringe magnetic field of an isochronous cyclotron comprising means defining an electrostatic field across a deflection channel at the extraction radius, the location of said field increasing in radius with respect to the center of the cyclotron; and magnetic material positioned inside and adjacent to at least a portion of said channel to reduce the cyclotron fringe field at the channel and to focus the beam of charged particles radially with respect to the center of the cyclotron, by concentrating the lines of magnetic force of said fringe field inwardly of but immediately adjacent to said channel to reduce said fringe field and then to reverse the normally decreasing field gradient in said channel.
 2. The apparatus of claim 1 wherein the means defining an electrostatic field includes a thin curved septum and a curved deflector electrode which define between them a shaped deflection channel with a high electric field gradient across it and the magnetic material is positioned along inside of at least a portion of said septum.
 3. An improved method for electrostatically deflecting a beam of charged particles at an extraction radius in the fringe magnetic field of an isochronous cyclotron comprising the steps of defining an electrostatic field within a channel at the extraction radius which increases in radius with respect to the center of the cyclotron; and placing a magnetic member along at least a portion of said channel to concentrate the lines of magnetic force of said fringe field inwardly of but immediately adjacent to said channel to reduce said fringe field and then to reverse the normally decreasing field gradient in said channel. 